Kimura S, Kakihata K, Sawada Y, Watanabe K, Matsumoto M, Hagiwara M, Tanaka H
Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan.
Department of Physics, Shizuoka University, Shizuoka 422-8529, Japan.
Nat Commun. 2016 Sep 26;7:12822. doi: 10.1038/ncomms12822.
The Bose-Einstein condensation is a fascinating phenomenon, which results from quantum statistics for identical particles with an integer spin. Surprising properties, such as superfluidity, vortex quantization or Josephson effect, appear owing to the macroscopic quantum coherence, which spontaneously develops in Bose-Einstein condensates. Realization of Bose-Einstein condensation is not restricted in fluids like liquid helium, a superconducting phase of paired electrons in a metal and laser-cooled dilute alkali atoms. Bosonic quasi-particles like exciton-polariton and magnon in solids-state systems can also undergo Bose-Einstein condensation in certain conditions. Here, we report that the quantum coherence in Bose-Einstein condensate of the magnon quasi particles yields spontaneous electric polarization in the quantum magnet TlCuCl, leading to remarkable magnetoelectric effect. Very soft ferroelectricity is realized as a consequence of the O(2) symmetry breaking by magnon Bose-Einstein condensation. The finding of this ferroelectricity will open a new window to explore multi-functionality of quantum magnets.
玻色-爱因斯坦凝聚是一种迷人的现象,它源于具有整数自旋的全同粒子的量子统计。由于在玻色-爱因斯坦凝聚体中自发形成的宏观量子相干性,会出现诸如超流性、涡旋量子化或约瑟夫森效应等令人惊讶的特性。玻色-爱因斯坦凝聚的实现并不局限于像液氦这样的流体、金属中配对电子的超导相以及激光冷却的稀薄碱金属原子。固态系统中的激子极化激元和磁振子等玻色子准粒子在某些条件下也能发生玻色-爱因斯坦凝聚。在此,我们报道磁振子准粒子的玻色-爱因斯坦凝聚体中的量子相干性在量子磁体TlCuCl中产生自发极化,从而导致显著的磁电效应。作为磁振子玻色-爱因斯坦凝聚导致O(2)对称性破缺的结果,实现了非常软的铁电性。这种铁电性的发现将为探索量子磁体的多功能性打开一扇新窗口。